Refrigerating apparatus



May 23, 1944. V Q MUFFLY 2,349,367

REFRIGERATING APPARATUS Original Filed Aug. 26, 1935" 8 Sheets-Sheet 1 INVENTOR May 23, 1944. G. MUFFLY 2,349,367

REFRIGERATING APPARATUS Original Filed Aug. 26, 1935 8 Sheets-Sheet 2 /IZS |25 /I24- INVENTOR May 23, 1944. G. lMUFFLY 2,349,367

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REFRIGERATING APPARATUS original Filed Aug. 26, 1 955 8 sheets-sheet 7 UME IN MINUTES O 0 60 /00 //0 o F2 24 j UME N MINUTES TlME )N MINUTES INVENTOR May 23, 1944. G. Mur-'FLY REFRIGERATING APPARATUS Original Filed Aug. 26, 1955 8 Sheets-Sheet 8 3&5

Patented May 23, 1944 REFRIGERATING APPARATUS Glenn Muiy, Springfield, Ohio Original application August 26, 1935, Serial No.

Divided and this application January 23, 1939, Serial No. 252,293

11 Claims.

This application is a division of my copending application, Serial No.` 37,789, nled August 26,

l 1935, now Patent No. 2,145,777, issued January This invention relates to -mechanical refrigerating mechanism and has relation to my copending applications for Letters Patent of the United States, Serial No. 697,124, filed November l 8, 1933, now Patent No. 2,145,773; Serial No.

and to provide a refrigerattng system of the type described having an improved support and spring mounting for the evaporators thereof.

Other objects of the invention are to provide a mechanical refrigerating system so constructed and arranged as to freeze bars of ice in such a manner that they are easily broken up into small blocks on natural fracture line; and to provide a triple valve of improved and simpli- 719,099, filed April 5, 1934, now Patent No. 2,- lo ed form for use in connection with a mechani- 145,774; and Serial No. 737,485, led July 30, 1934, now Patent No. 2,145,775, all of these having issued January 31, 1939.

One of the objects of the invention is to provide a refrigerating System control mechanism in which a single thermostatic element effects both the cycling of the` evaporators and the cycling of the condensing unit.

Another object is to provide flat surface evaporator units contacting with at surfaces of a water tank, which is adapted for the freezing of masses of ice on its inner wall, and to utilize the weight of the water tank together with that of the water and ice contained therein in a manner to increase the pressure between the evaporator surfaces and the tank surfaces contacted thereby to a value considerably in excess of that which is represented by the weight of the tank and its contents.

Other objects are to provide a refrigerating system so constructed and arranged as to effect control thereof by means of a single thermally responsive element associated with two or more refrigerant conduits; to effect the operation of the control mechanism between two temperature limits of which the higher limit is represented by cabinet air temperature and the lower limit is represented by refrigerant vapor temperatures; and to combine heat exchange means be tween two or more refrigerant conduits with 4d valve means regulating the flow of refrigerants in the system.

Other objects are to provide in a refrigerating system of the type described, an improved form of water tank and cover so arranged that the cover may be pushed backward in Aopening the tank and thus provide ready access to the tank without removing the cover; and to provide actuating and clamping means of novel form for the tank cover. A

Other objects are to provide a novel form of refrigerant evaporator unit having iins integral with the surface which contacts a water tank so that better and surer defrosting to 'free the ice blocks formed within the tank is obtained;

cal refrigerator ice maker employing three sets of evaporator units of which two are defrostmg while one is refrigerating for the purpose of making ice.

A further object is to provide an improved type of refrigerator cabinet, particularly adapted for use in connection with the type of ice maker above mentioned, and having an inner form conducive to the natural flow of air over the cold surfaces of the refrigerating system cooperating therewith.

'I'he above being among the objects of thev present invention the same consists in certain novel features of construction, combinations of parts, and step or steps of operation to be hereinafter described with reference to the accompanying drawings, and then claimed, having the above and other objects in view. h In the accompanying drawings which illustrate suitable embodiments of the' present invention and in which like numerals refer to like parts throughout the several different views.

Figure 1 is a fragmentary front elevational view cf a refrigerator cabinet, with door open, showing the cooling elements and control meehanism for the refrigerating system in place; Fig. 2 is a fragmentary vertical sectional view taken on the line 2-2 of Fig. 1, with the door closed and showing the cooling and control elements of the refrigerating system mainly in eievation, the water tank being partially broken away to disclose ice floating therein;v

Fig. 3 is a diagrammatic view of the refrigerating system employed in the construction illustrated in Figs. 1 and 2, showing the path of ow of the refrigerant:

Fig. 4 is an enlarged front elevational view of the control switch and valve mechanism shown in the previous views;

Fig. 5 is a view of the mechanism shown in Fig. 4, taken from the left-hand end thereof as viewed in Fig. 4

Fig. 6 is a view similar to that shown in Fig.

4, illustrating a slight modification thereof in which the two functions oi' the control mechain closed position;

Fig. 9 is a view similar to Fig. 8 but showing the switch in open position;

Fig. 10 is a partially broken, partially sectioned side elevational view of a control mechanism identical with that in Fig. 7, but connected with two bulbs instead of with one as in Fig. 7;

Fig. 11 is a partially broken, partially sectioned side elevational view of a modified form of valve mechanism adapted to control three evaporator sections instead of two; Fig. 12 is an enlarged view of the switch and ratchet mechanism shown in Figs. 7 to 10, inclusive, but modiiled for use with the triple valve shown in Figs. 11 and 13;.

Fig. x13 is a vertical sectional view of the mech- :mism shown in Fig. 11, taken on the line I3-I3 thereof;

Fig. 14 is a partially broken, partially sectioned top plan view of a valve and switch control assembly similar to that shown in Fig. 4, but employing a triple valve construction similar to that shown in Fig. 11;

Fig. 15 is a partially broken, partially sectioned side elevational view of the device shown in Fig. 14, with the cover 256 removed, showing parts 248, 250, 25|, and 252 in section on line I5'-I5 of Fig. 14, while the valve assembly below these parts is shown in section on line I5-I5 of Fig. 14;

Fig. 16 is a bottom view of the triple valve shown in Fig. 15, with the cover 24| removed;

Fig. 17 is a partially broken, partially sectioned side elevational view of a gear drive which may be substituted for the thermally actuated levers and ratchet devices seen in previous views for the purpose of actuating the valve mechanism on a timed cycle instead of on a thermally controlled cycle;

Fig. 18 is a horizontal sectional view taken on the line IB-I'B of Fig. 17;

Fig. 19 is a side elevational view, partly in section, showing a refrigerator cabinet and a slightly modiied arrangement of parts therein, including the cover mechanism for the tank, the fins in pairs integral with evaporator units, and rounded sharp freezer to allow better air flow;

Fig. 20 is an enlarged, partially broken, partially sectioned side elevational view of a fragment of the structure shown in Fig. 19, showing a section through one of the evaporator units to illustrate the integral iin construction;

Fig. 21 is a sectional view taken on the line 2I-2I of Fig. 20, showing the rocker shaft and spring support for the evaporator umts;

Fig. 22 is a more or less diagrammatic view showing a block of ice as it might be frozen during a prolonged period of operation on one section of the evaporator shown in Figs. 19, 20, and

. 21, illustrating the lines of easy fracture;

Fig. 23 is a diagrammatic representation of a hook-up suitable forv operation of three evaporator sections in a refrigerating. system by means of a triple valve mechanism;

Fig. 24 is a graph showing typical temperature curves of a dual valve refrigerating system having two evaporator sections for ice making and :gisting a separate thermostat such as seen in Fig. 25 is a similar graph showing curves for a system using the type of control seen in Figs. 4, 7, and 10, with an idle period following each freezing period;

Fig. 26 is a graphic chart of temperatures obtained in a triple evaporator ice maker employing a triple valve which is actuated independently of the thermostatic switch, as by the gear drive seen in Figs. 17 and 18. or with the thermally actuated -triple valve and a separate ther- `mostatic switch controlling the operation of the motor which drives the compressor;

Fig. 27 shows a fragmentary vertical sectional view taken through a form of refrigerator cabi- A net particularly adapted for promoting a thermal circulation of air suitable for the functioning of the type of refrigerating systems shown in the preceding views, the cabinet having its liner rounded at the rear upper corner to Just clear the rear of the water tank cover when it isv pushed back for access to the tank;

Fig. 28 is a vertical sectional view taken through the cabinet shown in Fig. 27 as on the line 28-28 thereof, showing how the cabinet liner is rounded at the top of each side to facilitate air flow over the tank and ns and to avoid the warm upper corners found in most refrigerators;

Fig. 29 is a fragmentary top plan view of the refrigerator cabinet shown in Fig. 27, showing the curvatm'e of the inverted L portion of the door;

Fig. 30 is a fragmentary vertical sectional view' taken through a modified form of cabinet structure in which the insulation is curved along with the cabinet liner and a removable condensing unit occupies the space between the insulation and the outer shell;

Fig. 31 is a top view of the structure shown in Fig. 30 with the cover 346 removed, showing the arrangement of the condensing unit therein;

Fig. 32 is a fragmentary vertical sectional view taken on the line 32-32 of Fig. 30; and

Fig. 33 is a fragmentary front elevational view of the cabinet shown in Figs. 30, 31, and 32, illustrating the form of door employed. I,

The present invention deals particularly with mechanism for continuously producing a supply of artificial ice and while the invention in -its .broader aspects is capable of application to refrigerating units of any desired size, it is particularly adaptable to those sizes of devices employed for domestic purposes and for that reason the illustrative embodiments of the invention herein shown and described are in connection with such types of refrigerators.

.As in the case 'of my previous patent applications above identied, the present invention is in connection with an apparatus by means of which masses of =ice are formed on one or more submerged walls or wall areas of a water tank located within a refrigerator cabinet of the domestic type, and means are provided for .periodically discontinuing the refrigeration of such surfaces or surface areas whereby the vice formed thereon may melt free therefrom and float upwardly in the water within the tank, whereby upon resumption of the refrigeration of such walls or wall areas additional masses of ice will be again frozen thereon to be later freed therefrom and float upwardly in the water of the tank to co-mingle with the ice previously frozen. By

this type of apparatus a constant supply of small individual masses of ice may be continually maintained in the water tank from which they may be readily dipped as desired whenever required for use. Additionally, the water itself is maintained at a V relatively low temperature. Thus, the construction and arrangement is preferably such that the body of water in the tank does not itself attain a sufficiently low temperature to cause it to be frozen as a whole and as a result the individual masses of ice caused to be formed and to float upwardly therein are maintained in a relatively free condition with respect to each other which permits their ready removal and use. Because of the fact that the bulk of the water in the water tank does not drop in temperature sufficiently to freeze the entire body thereof, the ice thus formed will continue to melt slowly, but it will be understood that any ice thus melting serves to replenish the main body ofv water from which the masses of ice are formed and, therefore, it is only necessary to replenish such water in the tank as may have been removed through -ice actually removed from the tank, orwater withdrawn from the tank for drinking or other purposes. I

In order to admit of proper sanitation of devices of the type described and particularly where employed for domestic purposes, it is important that the water tank be readily removable for cleaning purposes and proper provisions are made to this end in accordance with the present invention.

It will also be understood that in refrigerators of the types herein under discussion, such refrigerators comprise a cabinet affording a suitably heat insulated chamber within which articles of food or the like may be stored for their-proper preservation. Heat is extracted from the chamber by means of a suitable refrigerating mechanism and while, in the broader aspects of the present invention, the particular type of refrigerating system is immaterial, that is to say whether it is of the mechanical compression type or of the absorption type, the former is shown by way of simplicity of illustration. In such a type of refrigerating mechanism it willbe understood that a suitably driven compressor is provided for compressing the expandedand gasied refrigerant and discharging the same to a suitable condensing unit where, under the influence of pressure and reduction of temperature, the refrigerant is changed to its liquid phase. The liquid refrigerant from the condenser, or from a receiver when associated therewith,. is

ice thereon. All the evaporators or evaporator sections are successively subjected to such a refrigerating eil'ect and subsequent rise in temperature 'sothat all combine to provide an approximately continuously replenished supply of ice in the tank. y

One of the main features of the present invention is the provision of a mechanism of the type described and control means therefor by the use of which not only is refrigeration of a par ticular evaporator or evaporator unit discontinued by stoppage of the flow of refrigerant through it during continued operation of the refrigerating system so as to permit the ice formed on the associated wall or wall area of the tank to melt free therefrom, but additionally to conducted in liquid state to one or more suitable evaporators where the pressure upon it is reduced and it is permitted .to expand, thereby to absorb heat, and when it has been so expanded or gasifled it is thereupon returned to the compressor where it is again compressed and its heat content extracted or reduced.

In accordance with the present invention the evaporator assembly is made up of a plurality of individual evaporators or evaporator umts, and means are provided whereby but one section of said evaporator or evaporator units is refrigerated at one time, the remaining sections or evaporator units being allowed to absorb heat during such time whereby to insure any ice which may have formed on the associated wall or wall areas of the water tank melting free from such wall or wall areas and be displaced therefrom, thereby to condition such wall or wall areas for the freezing of additional masses of insure idle periods of the refrigerating system augmenting the warming period of each individual evaporator or evaporator unit.

Another feature of the present invention is the provision of a simplied water tank structure and evaporator or evaporator unit for cooperation therewith for the purpose described, resulting in a simplified construction more economical to manufacture than in the constructions disclosed in my prior applications above identied.

The control means operable to extend the warming up periods of the individual evaporators or evaporator units also forms an important feature of the present invention as do a number of other individual features of construction and arrangement of parts that will now be specifically described.

l Referring to Fig. 1 a refrigerator cabinet 5l is shown with the door opened or removed and a considerable part of the cabinet broken away. The ice and water tank 53 is.r broken away to show only its outline so that the control parts located behind it are visible. Below the tank is the sharp freezer 54 which is provided with insulated walls and with the insulated door 55. It is supported by the hangers 56 which also support rocker shafts 51, which in turn support the ns 58 which are part of the evaporator units contacting the two angularly disposed at surfaces 59 of the tank 53. It will be understood that the liquid refrigerant is iirst discharged into the low pressure side of the system in the evaporating means associated with the sharp freezer 54, and is then conducted to the evaporator units of the ice making part of the system.

The evaporator units 60 (Fig. 2), of which' live are located on each side of the tank, are each formed with two lrectangular contact areas 62 (Figs. 1 and 3) which contact the at angularly disposed walls 59 of the tank to thereby Asupport it. It will be seen that-the surfaces 59 are disposed atangles of less than forty-five degrees from the vertical, hence the tank by its wedging action between these surfaces, Awhich support it, will bear upon the surfaces B2 with a total force considerably in excess of the proportionalweight of the tank and its contents, thus insuring a good thermal contact between the tank and the evaporator units. Furthermore, because the units 60 are pivoted on the rocker shafts 51, and because the walls of the tank 53 are preferably formed from thin metal, the units may rock and the walls yield to insure full area of contact between all the areas 62 and the surfaces 59 of tank 53.

Due to the V formation of the lower part of the removable tank 53, it may be advisable in some cases to provide a support for tank 53 to make it more stable in its upright position when removed from the cabinet. One method of doing this is to attach the false front 13 to the tank 53 as seen in Fig. 2. lThis front plate .has a width substantially equal to that of the tank to which it is rigidly attached and with which it is removable from the cabinet. Being substantially flush with the bottom of the tank, this plate prevents sidewise tipping of the tank when placed on a fiat surface such as a table top. I

'Ihe door 52 (Fig. 2) is of the inverted L type which I have disclosed in copending applications hereinbefore identified. One of the refrigerant inlet manifolds 6| supplies the various evaporator units 60 on one side of the tank 53 with refrigerant of which a substantial part is still in the liquid phase, although under low or evaporating pressure.r This refrigerant evaporates in the various evaporator units 60 on such side of the tank 53 and exits through the corresponding outlet manifold 63. Refrigeration of the evaporator units 60 causes heat to be extracted from the contacting walls of the tank 53 and from the water immediately adjacent such wall areas so as to cause such water to be frozen into ice. After ice has been frozen on the inner side of one of the angular walls 59 of the tank 53 the control acts to stop refrigeration so that the ice blocks may be melted free from the wall by means of heat picked up by the fins 58 from the air within the cabinet. In the meantime refrigeration will be produced in the evaporator units contacting the other angular wall 59 of the tank, as will be explained in more detail in connection with following views.

Fig. 3 shows diagrammatically the relationships between various parts seen in Figs. l and 2 and includes a representation of the high side" or condensing unit of the system. Refrigerant flow may be traced in Fig. 3 as follows: Refrigerant vapor leaving the left-hand manifold 63 passes through the tube 64, which contacts the bulb |03 of the control |0|, to the coil 68 of the the stem 1I. This would change the path of rel frigerant, causing it to flow from the T 91 through the right hand manifold 6| and the right hand set of evaporator units to the tube l5 and thence through the tube 61 of the heat exchanger 66 and the tube 69 to the valve port opened by the valve 83.

The rocker 16 of valve assembly 15 is actuated by means of spring pressure upon the point 1I or by mechanical means energized by control |0|, as will hereinafter be explained in more detail. The control |0| also actuates a switch for closing the circuit through motor 81 by effecting contact between line wire and motor wire ||0. 'Ihe other line wire |l2 leads directly to the motor 01.

In Fig. 4 we see an enlarged detail view showing how the valve assembly 15 and the control assembly |0| are associated so that the former is actuated by the latter. For the sake of simplicity the thermostatic bulb |03 is shown contacting tubes 69 and 10 instead of tubes 64 and 66, thus omitting the heat exchanger 66 from this figure.

Valve 82 is shown open, hence refrigerant vapor is passing from the tube 10 to the tube 1| in the same manner as illustrated in Fig. 3. The circuit comprising wires ||0 and is closed, as seen in Fig. 4, due to the bellows |04 of the control |0| being expanded so, that the arm |03 has swung upward on its pivot |06, compressing the spring .|01 and tilting the mercury bulb switch |09 to its closed position. The compression of spring |01 is adjusted by means of a screw |09 to vary the temperatures at which switch |09 is opened and closed. The bellows |04 is responsive to the vapor pressure in the bulb |03 which is partially filled with a volatile liquid in accordance with conventional practice, and

heat exchanger 66 and after passing through this coil is lead by tube 10 to the valve assembly 15 into which it is free to pass because the valve 82 is lifted from its seat. This allows the refrigerant vapor to enter the housing 8| of the valve assembly, from which it exits through tube 1| tothe suction side of compressor 86.

After refrigerant vapor has been compressed by the compressor 85 it is discharged through the tube 88 to the condenser 89, where it is liquefied and then drained into receiver 90. The liquid refrigerant leaves'the receiver through tube 9| and passes through the helically wound tube 92 gxzinected with the bellows by means of the tube Since it is considered that cold refrigerant vapor is passing through the tube 10, the vapor pressure in bulb |08 and bellows |04 is being gradually reduced so that finally the spring |01 will overcome the expansive force of bellows |04 and allow the' arm |05 to tilt downward until the circuit including wires ||0 and is broken of heat exchanger 66 in counter flow association with the vapor tubes 61 and 68. The liquid gives up a considerable part of its specific heat to the vapor in the active tube 68 and then passes throughl the tube 93 to the pressure reducing device 94, which may be an expansion f valve, a capillary restrictor, a float valve or equivalent device.

The liquid refrigerant, now under reduced pressure, enters an evaporating coil (not shown) in the sharp freezer 54 from which it exits in partially evaporated state through tube 96 to the 'i' 91 at which point it is free to pass into whichever one of the manifolds 6| is active at the moment. It will be seen that if the rocker arm stem 18 of the valve assembly 15 were moved to the left about its pivot 11 by an angular pressure upon the point .19, the valve 82 would be closed and the valve 83 would be opened, since they are both by the mercury switch |09. Before the downward movement of arm |05 has caused the switch |09 to open it will have moved downwardly far enough to allow the push rod |2| to let the arm |23 rock in a clockwise direction under influence spring |24, raising the pin |26 at4 the left end of rocker |23 and in turn lifting the pawl |21 until it falls into engagement with the next higher tooth of ratchet wheel |28.

After the circuit is broken in the switch |89 of control lol, the motor s1 win be idle, hence no refrigerant will be drawn through any of the units and no refrigerating effect will be produced upon the bulb |03, which consequently warms up, approaching the temperature of the .Y air within the cabinet while this air temperamounted upon the valve rocker 16 associated ywith 'l5 ture itself is also rising due to the stoppage of active refrigeration. This rise of temperature of the bulb |03 produces an increased vapor pressure within the bulb and vapor passing from the bulb through the tube |02 to the bellows |04 causes the bellows to expand, compressing springs |01 and |24. The upward push of the bellows transmitted to the rocker |23 causes it to move in a counterclockwise direction about its pivot |25. 'I'his exerts a downward push on the pawl |21 causing the ratchet wheel |28 to move in a counterclockwise direction upon.the xed stud |29. The cam or star wheel |30 is secured to the ratchet wheel |28 and is rotated thereby upon the stud |29.

In the position shown in-Fig. 4 the star wheel |30 is located with a tooth pointing toward the roller |3| at the right while the roller |3| at the left has moved nearer to the star wheel |30 and is located between two teeth thereof. The spring |33, which is broken away in Fig. 4 but seen in full in Fig. 5, is compressed between the adjustably fixed point |34 and the movable point 19 of the valve rocker stem 18, thus holding the valve 83 against its seat. The roller |3| at the left of star wheel |30 is not contacting the star wheel, but there is a very small clearance between these parts so that the star wheel |30 need be moved but a few degrees before it contacts the roller |3| and begins to move the fork |32 which is rigidly attached to the valve rocker stem 18.

During the idle period of the condensing unit the bellows |04 is expanding, as before explained, and this producs the movement of star wheel |30 which causes the valve stem 18 to move to the left until it passes the center line and the spring |33 causes it to move farther to the left until stopped by the engagement of valve 82 with its seat. Since the ratchet wheel |28 has ten teeth and the star wheel has ye teeth, a movement of one tooth on the ratchet wheel will bring a space of the star wheel in line with the right hand roller i3! so that the next downward movement of the pawl |21 will cause the valve mechanism to snap back to the position shown in Fig. 4. The stem 18 is soldered or otherwise sealed to the flexible meta-l bellows 85 which is in turnsoldered to the upper portion of housing 8|, which is made gas-tight with a gasket. l

It will be noted that bracket |36 for pointed screw |34 is attached to part |35 by means of two screws and that it is slotted for the upper screw, making the point adjustable sidewise on an arc about the lower screw. This provision is made so that the dead center line of spring |33 may be varied to obtain equal temperatures of operation for the movements to left andto right of the fork |32. Such an adjustment has been found highly desirable in equalizing the lengths of idle periods after freezing on the right side and after freezing on the left side. The point |34 is also adjustable vertically to vary the compression of spring |33, thus providing an additional adjustment of the temperature at which the valve mechanism is operated.

Fig, 6 illustrates a slightly modified ,arrangement of parts by means of which the function of the switch mechanism and of the valve mechanism may be separated to produce cycles of the ice maker independently of, the cycles `of condensing unit operation produced by a conventional thermostatic switch. The supportingr member |35 is the same as in Figs. 4 and 5 and v supports some of the sameV parts thereon, but is arranged differently in some respects and inoludes additional parts. The thermostatic switch |54, its tube |53, and the bulb |52 perform their usual functions of opening and closing contacts between the wire I and the wire in vresponse to temperature changes of the bulb |52,

which is preferably loca-ted where it is affected by the temperature of air within the refrigerator cabinet.

The bulb |40 replaces bulb |03 of Fig. 4 in contact with tubes 69 and 10, causing bellows |42 to expand and contract with the changes of vapor pressure of a volatile liquid within the bulb |40.`

When the tube 10 drops in temperature, due to the start of frost-back from the evaporator assembly with which this tube is associated, the bulb |40 is chilled and the bellows |42 contracts under the force of spring |41 which is powerful enough to turn the ratchet wheel |28 through the medium of the pawl |21, thus snapping the valve mechanism to the left and opening valve 83 (Fig. 4). This action takes place during operation of the compressor and shifts the refrigerating effect to the opposite side of the tank independently of the thermostatic switch |54.

'I'he closing of the valve associated with tube 10 (82 in Fig. 4) stops the iiow of cold refrigerant through tube 10 andallows bulb |4'0 to warm up, approaching the temperature of air within the cabinet, which expands bellows i 42 and recompresses spring |41, lifting pawl 21 into a new notch of ratchet wheel |28. After the freezing operation has been completed on the side of the tank now refrigerated the tube 69 will drop intemperature due to the start of frost-back" and cause the bellows |42 to contract again, snapping the valve mechanism back to the position which allows now of refrigerant through the tube 10 and closes the outlet port of the tube 69'. In either Fig. 4 or Fig. 6 the bulb (|03 and |40 respectively) might be in thermal contact with the assembly 15, say on bottom cover ofthe housing 8|, instead of contacting the two tubes 10 and 1| The eect is Asubstantially the same, but slightly delayed, which calls for a slightly different adjustment of the control.

The screw |48 and its lock nut |49 are provided for the purpose ofv adjusting the compression of the spring |41 to obtain the desired cycles of operation. The strength of the spring |41 and the setting of the screw |48 should be such that the valve mechanism will be actuated before enough frost has accumulated to interfere with the action of the bellows 85 or to represent a material loss of refrigeration to the suction line 1|. On the other hand, thesetting of the screw |48 and the strength of the spring |41 must be such that the pawl |21 is lifted into engagement with the next tooth of the' ratchet wheel |28 during the warm-up period which follows each switch of the valve mechanism and before the freezing on the new side has progressed far` enough to again start the frosting-back which causes bellows contraction. The cycle of operation produced by a control as seen in Fig. 6 is further explained by the graph shown in Fig. 24. In Fig. 7, the bulb |03 is associated with the two tubes 69 and 10 for the same purpose as in Fig. 4, 4but in this view the tubes are shown coiled` in parallel around the bulb |03. The bellows |60 acts in the same manner as the bellows |04 of Fig. 4, but is shown in inverted position and connected with a different mechanism, employing open contacts instead of the enclosed mercury type of switch shownv in Fig. 4. The types of switch mechanisms and contacts might vary greatly without departing from the spirit of this invention, hence I show only two types of switches; the mercury bulb type, which may be actuated by a slow movement, and a, spring-snap type, which produces a sharp break of the current by mechanical means. It will be understood that I do not limit myself to the particular mechanism shown in this respect.

Fig. '7 will nt into the diagrammatic view of Fig. 3 in the same way that Fig. 4 does, with the heat exchanger 66 omitted in this case because the single heat exchange coil 92' carrying warm liquid refrigerant through the housing |88 has been added. In the sectional portion of Fig. 7 the plane of section of the bulb |08 and o f the two tubes coiled around it is taken at the rear of the plane of the section through the two valve ports and parts 92 and' 589 in order that the incoming ends of the tubes 66 and 10 may be shown as behind the vertical legs of the same tubes which connect with the ports controlled by the valves 82 and 83. It will be understood that the bulb |03 responds equally to temperature drops of the helically wound portion of the tube 60 and to temperature drops of the helically wound portion of the tube 10, being exposed to an equal length of each at a uniform distance therefrom. The action is the same as in Fig. 4,'where the bulb |03 contacts an equal length of each o the tubes 69 and 10.

When the bellows |60 contracts under pressure of the spring i6| in response to a drop of temperature of the volatile liquid in the bulb lr03, the stem |64 moves upward with respect to the retaining wall |63 and the ten tooth ratchet wheel |66. The spring |66 is thus moved from the position seen in Figs. '7 and 8 to the position shown in Fig. 9. When the spring |65, in its upward travel, falls ofi of the tooth against which it is bearing on the ratchet wheel |86 it strikes the end of the push rod |16 causing it to slide to the right in its bearing |16 and strike the leaf spring |10 which moves it to the right, causing the contact |12 to snap away from the contact |13 against which it has been bearing vunder action of the spring |10. Contact |13, supported by the rigid arm |14, remains xed while the contact |12 moves away x.from it. The arm |16 is electrically insulated by being supported by the insulating block |1|, but the contact |13 and the conductor may be insulated from arm |16 instead if desired. Likewise the contact |12 and the conductor may be insulated from the spring by means oi a washer and a bushing of non-conducting material.

The electrical connection between the conductors ||0 and is broken by the contraction oi' the bellows |60 in exactly the same manner that the contraction oi the bellows |06 in Fig. 4 breaks the circuit therein, although through the medium of a different mechanism. Likewise, the expansion of the bellows |60 due to stoppage of refrigeration will cause the opening of the valve 83 and the closing of the valve 82 as in the case of Fig. 4, through the medium of mechanism described below.

As the bellows |60 (Fig. 7)" expands due to stoppage of refrigerating effect in both of the tubes 69 and 10 and because ofthe rise of air temperature resulting from stopping the compressor 86 (Fig. 3) it compresses the spring |6|, moving the stem |66 and flat spring |65 downwardly from the position shown inl Fig.v 9 to the position shown in Fig. 8, rotating the ratchet wheel |66 and the gear |8| which is fixed for equal rotation with the ratchet wheel |66, onetenth of a revolution. During this rotation a tooth of the ratchet wheel |66 engages the lug |11 on the end of the spring |10. holding the contact |12 away from the contact 13, and at the end of the 36 degrees of rotation the lug |11 drops into the next notch in the ratchet wheel |66, allowing the contact |12 to touch the contact |13, reclosing the circuit, which starts the motor 81 (Fig. 3) and operates the compressor.

During this counter-clockwise rotation of the gear |8| it has been rotating the piniony |82 with 75 which it meshes. 'I'he ratio o! teeth on the gear to teeth on the pinion is ve to one, hence during 36 of gear movement the pinion will have moved or one-half of a revolution in a clockwise direction. It will be noted that no movement of the ratchet wheel |66 has occurred between Figs. 8 and 9 and since the only change has been the upward movement of the spring |66 and the resulting openingv of the switch. During the next downward movement of the spring |66 to the position shown in Fig. 8, the ratchet wheel |66 and the gear 8| will have been moved, bringing the crank pin |83 fixed to the pinion |82 and the connecting rod I 84 to their extreme leftward positions (not shown), which will cause the rocker arm |88 (Fig. 7) to pivot upon its bearing concealed within the bellows |81, moving the point |88 to the extreme right, and carrying with it the lower end of the spring |33, which then acts upon the point 19 of the valve rocker 16 to open the valve 83 and close 4the valve 82.

The action is similar to that explained in connection with the construction illustrated in Fig. 4, in that the expansion of the bellows due to non-refrigeration of bulb |03 causes the valve mechanism to move, opening one valve and closing the one that has been open and then closing the switch, while the cooling of the bulb |03 which results from the closing of the switch and completion of an ice-forming period causes the bellows to contract until the pawl (here represented by the spring |65) falls into the next notch of the ratchet wheel and the circuit is opened.

The spring |6| (Fig. "7) is provided with an adjustable seat' at its lower end on the nut |62 which has a threaded engagement with the member |63. The spring forces effective upon the movable end of the bellows |60 is thus adjustable for regulation of the cycles produced by this control mechanism. If desired, an additional spring or leverage adjustment may be provided in any of the well-known forms of such mechanisms for the purpose of making the temperature adjustments for range and for high and low limits separately and independently.

Fig. 10 is a duplication of Fig. '7 with the exception that some details have been omitted and the coils of tubes 69 and 10 are shown as separately coiled, one about bulb |89 and the other about bulb |98. Both bulbs are connected with the same bellows |60. I'his view is shown to illustrate a principle which may be employed in connection with a control of the nature described. In such a construction and with a charge of volatile fluid which is more than enough to ll one bulb in the liquid phase the bellows will respond to the temperature of the warmer bulb. exactly as if the other bulb were not connected; and with a charge of volatile iluid which is small enough so that all of the liquid portion may be contained in one bulb the bellows will respond to the temperature of the colder bulb exactly as if the other bulb were not connected. Where there are more than' two bulbs connected to a single bellows and the liquid charge may be contained in any one bulb, the bellows will respond to the temperature of the coldest bulb, since that is where the liquid will be and the vapor pressure is established by the warmest liquid in the system as soon as equilibrium is established. v

Should there be only one large bulb and one small bulb connected with the same bellows and the liquid charge be more than enough to fill the smaller bulb and less than enough to till the large bulb the result would Be that the bellows would always respond to the temperature of the larger bulb no matter which of the bulbs were the colder, for the liquid-vapor contact wouldl always be in the largerbulb.

From the above it will be clear that the ccnstruction shown in Fig. will operate in exactly the same manner as that shown in Fig. 7, expanding the bellows in accordance with the rise of air temperature when neither tubes 03 nor 10 are refrigerated and contracting the bellows in accordance with the ltemperature of the colder of the two tubes. This principle applies equally to a system in which three bulbsv are connected with one bellows, so long as any one bulb will contain all of the volatile liquid with which the connected bulbs and bellows are charged.

It will thus be seen that there might be three suction tubes instead of the two (33 and 10), with three bulbs instead of the two and |93), and that the bellows |30 of Fig. 10 would act in response to the vapor pressure established by the coldest of the three bulbs. Such a system will be described later in connection with Fig. 23, where three separate suction lines (23|, 232, and 233) have three separate bulbs (32|. 32B, and 323) associated with them and with a single control bellows.

Bulbs and |99 are separately adjustable vertically to vary the iniluence of tubes coiled around them. Slotted ears |93, screws |34 and extra tapped holes are provided for this purpose. This adjustment compensates for any inaccuracies in the valve mechanism or differences between the two evaporator sections` as does the adjustment of part |33 inrFigs. 4, 5, and 6.

Fig. 11 is a sectional view througl the axis of a valve mechanism designed to control three suction passages in place of the two passages (tubes 89 and 10) seen in previous views. The operating mechanism seen at the right of Fig. 11 is shown in Fig. l2, which may b'e considered a modified detail of Fig. 10 with nine teeth on the ratchet wheel instead of ten. Fig. 13 is a section of Fig. 11 on the line I3|3 thereof and conversely Fig. l1 is taken on line |l|| of Fig. 13.

Referring to Figs. 11 and 13it is seen that there are threefvalves 2|1 carried by the tilting spider 2|0, which is pivoted upon the ball 2|3 The shaft 200, upon whichgthe pinion 204 is rigidly mounted, is thus turned through each time that the bellows I 30 expands during an idle period of the compressor 80, seen again in Fig. 23. Since this shaft 205 lcarries the arm 201, to the outer end of which one end of the spring 203 is connected by ball-and-socket Joint,c

it 'will be understood that at the end bf each 120 movement of the arm 201, caused by an expansion of. the bellows, the arm and the spring come to-rest in a position which holds one of the three valves 2|1 open and the other two closed. At each 40 movement of the ratchet C wheel the outer end of the spring 203 moves 120, Icausing the open valve 2|1 to snap shut and another of these three valves to open. Thus, hnly one of the three suction tubes 22|, 222, and 223 is open to the interior of the housing 2|0 at a time and the refrigerating effect produced by this tube on one of the three bulbs will cause the next contraction of the bellows |00.

Warm liquid refrigerant, passing through the tube 02 coiled within casing 2|. (Fig. 1l) gives up some of its heat to the Icold vapor which enterst through the open valve and exits to the suction tube 1|, thus maintaining the housing 2|! and associated parts at a temperature which of the stem 2|4 mounted upon the xed spider y 2li, and that for any given position of the arm 201 and the spring 200 there is but one of the valves 2|1 lifted from its seat while the other two are held closed by the spring 200.' .x

'I'he arm 201 is carried upon a shaft 203 (Figs.

11 and 12), which is actuated by the pinion zu.

best seen in Fig. l2. The ratchet wheel 20| is actuated in the same manner as the ratchet wheel |66 shown in previous views, but it has nine teeth in place of ten, hence the shaft 202, with which the ratchet wheel 20| is rigidly connected, turns one-ninth of a revolution or 40, instead of 36 as in the case of shaft |61 in Figs. '1, 8, and 9 during each expansion of the bellows.

The switch parts in Fig. 12 operate exactly as described in connection with Figs. 1, 8, and 9,

but the gear 203 turns 40 during each Warnung up period. The pinion 204, driven by the gear 203, has one-third as many teeth as the gear, hence for each ratched tooth of 20| the pinion 204 makes one-third of a revolution.

prevents excessive frosting of the bellows 2|I, thus insuring that the bellows retains its flexibility.

The housing 2|8 is secured with bolts or suitable holding means to the wall 2|2 which sup- Y' ports the valve assembly, and a. gasket` between these parts makes the housing gas tight. The operation of a triple valve mechanism such as is seen in Figs. 11, 12. alia 13 by a beuows tueii as seen in Fig. 10, but with three bulbs and three suction tubes is believed to be well explained above, but for further clariilcation I show a slightly modiiled assembly in Figs. 14, 15, and 16.

The valve assembly 230 seen in Figs. 14,15,

and 16 is quite similar to the one shown in thei three preceding views, but the spring 245` (Fig. 15), under compression, replaces the tension spring 203 ot Fig. 1l and the operation is effected without the use of gears.

Referring to Fig. 15 it will be noted that thel bulb 260, secured in intimate contact with the tubes 23|, 232 and 233 by means of the clamp 26| is .connected through the tube 232 to the interior of the bellows 233. This arrangement includes a charge of volatile fluid of such volume that the entire liquid portion of the charge may be contained in the bulb 260, hence the bellows 203 will have an internal pressure equal to the I vapor pressure within the bulb 260. VThe result, as before explained, is the same as if there were three bulbs 200, one contacting each of the three tubes 23|, 232, and 233, with the same quantity oi' volatile liquid and with all three bulbs connected with the interior of the bellows.

As shown in Fig. l5, the circuit including the wires ||0 and isopen at the switch 261 and the bellows 263 is contracted, as would ben the case immediately after the completion of a freezing period by the evaporator section connected with the tube 23|, which is shown with Athe valve 234 open so that refrigerant vapor is free i to pass into the housing 24| of "the valve mechanism and out through the tube 1 to the'suction side of the compressor.-

The refrlgerating effect of the tube 23| upon 'the bulb 260`has just caused the opening of the switch 261 and the bulb 250, being no longer refrigerated, will now warm up, approaching the temperature of air within the refrigerator. The resulting expansion of the bellows 263 will move the arm 254 upward at the right end, pushing downward on the pawl 253, which engages one of the three holes in the top of the ratchet wheel or disc 252, as shown in the plan view in Fig. 14. The relationship of these parts is such that the disc 252 will be moved in a counterclockwise direction as viewed in Fig. 1li something more than 60 and less than 120 before the arm 255 has tilted the switch 251 to the position which recloses the circuit and starts the motor. The movement of the disc 252 and shaft 250 causes the farm 252 and the point 251 to move correspondingly. since the arm 242 is secured to the shaft 250 by means of the set screw 229.

In any of the foregoing views, Figs. 4, 7, 10, 14, l5 and Fig. l1 with reference to Fig. 10, the switch might be shorted by connecting wire lll to wire ll l, or separating the switch as in Fig. 6. The ice making periods would then follow each other .consecutively in accordance with Fig. 24, which will be described later.

After the point 241 has been moved something more than 60 and less than 120 and before the switch 261 has reclosed the electrical circuit, the spring 245 will have assumed an angle at which it will cause the stem 253 to tilt upon its pivot point 238 to close the valve 235 and open the valve 235 (Fig. 16). The release of the spring pressure acting against the pawl 253, will under normal conditions, allow enough additional expansion of the bellows 253 to immediately move the switch 261 to the closed position, but in any event the switch will close soon afterl the valve mechanism has snapped to the new position.

The snapping over center of the spring 245, which is held in place solely by its pressure against the cups 246 which engage the two points of 243 and 241, will normally cause the ratchet disc 252 to move ahead, away from the propelling pawl 253, to find a new point of rest midway between thel two valves which it is new holding closed. Contraction of the bellows 263 caused by the cooling of the tube 232 which connects with the now open valve 235 and with the active evaporator section will gradually tilt the switch 261 toward the open position and will meanwhile lift the pawl 253 until it falls into the next hole in the top of the disc 252. The adjustment must be such that the pawl falls into the next hole before the switch closes the circuit again, as otherwise the next freezing period would be initiated in the same evaporator section which was last active.

At the third cycle of compressor operation the cooling effect will be on the third evaporator sec` tion with the valve 236 open and the bulb 260 Will be cooled by the .tube 233. the spring 265 by means of the screw 266 allows for setting the temperatures of operation. The control assembly 255 is provided with a cover 256, which is removed in Fig. 15. 'I'he wall 240' supports the valve mechanism and the housing 24| is secured thereto by means of screws with a gasket to insure a gas tight t.

As in the case of the dual valve and two evaporator section designs, itis also permissible to separate the thermostatic switch from the valve actuating means, by merely taking the switch out of assembly 255 and providing a separate thermal switch. as is done in Fig. 6.

I'he adjustment of This would change the cycle of operation to that illustrated by the chart shown' in Fig. 26, whereas the cycle produced by a control of the type shown in Figs. 14, 15, and 16 is similar to that shown by the graph in Flg. 25, except that another curve would be added to F and G to represent the third evaporator section.

Another method of separating the ice-makingV cycles from the thermostatic control of the condensing unit (motor and compressor) is to employ time actuated means as illustrated in Figs. 17 and 18 to control the refrigerant valves in the two or more suction passages and to add a separate thermostatic switch of conventional type to control the motor.

Referring to Fig. 17, the motor 210 drives the vertical shaft 21| on which there is a worm 212 driving the worm wheel 213, which is free to rotate upon the fixed horizontal shaft 214 (seen in Fig. 18). The lplanetary shaft 219 has its bearing in the worm gear 213 and keyed to this shaft, which is free to rotata in the worm wheel 213, are the gear 213 on one end and the gear 280 on the opposite end. The gear 218 meshes with the fixed gear 211 and is driven thereby as the shaft 219 is carried around the fixed shaft 214 by the worm gear 213. The gear 280, being keyed to the same shaft as gear 218, rotates with it and drives the smaller gear 28| (Fig.y 18), which is free to rotate upon the fixed shaft 214.

By selecting suitable numbers of teeth for these four spur gears it is possible to obtain a very great ratio of speed reduction between the worm wheel 213 and the driven gear 28| with its extending shaft 282 to which the arm 283 is keyed. Assuming that the fixed gear or pinion 211 has seventeen teeth; that gear 218 has thirty-two teeth; that gear 280 is of a finer pitch and has forty-nine teeth; and that the driven gear or pinion 28| has twenty-six teeth; the speed reductionmay be calculated as follows:

which means that the gear ratio is only a trifle over one to one. It is obvious that a ratio of one to one would make the gear 28| stand still with reference to the stationary gear 211. Instead of standing still the gear 28| does make .0012 of a revolution for each revolution of the worm wheel 213, or in other Words it revolves at la of the speed of worm wheel 213. By employing a single threaded worm 212 with eighty teeth on the wheel`213 a reduction of eighty to one is obtained,I making the total ratio of speed reduction 66,640 to 1.

Assuming a motor speed of 1750 R. P. M. it will be found that the gear 28|, shaft 282, and arm 283 will make one revolution in approximately thirty-seven minutes. When this period is divided into two parts, as in the case of a dual evaporator ice maker, 'employing a valve mechanism as shown in Fig. '7 with gear |82 mounted on shaft 282 of Fig. 18, it will provide about eighteen and one-half minutes of freezing time and an equal length of melting or ice-freezing time for each of the two evaporators of the ice maker. Should the shaft 282 be employed to drive the shaft 250 of Fig. 15 with no further gear reduction it would provide one-third of thirty-seven minutes, or twelve and one-third minutes of duration for forming ice with each of the three evaporators (see Fig. 23 for diagram of pipe connections). This latter combination allows'twenty-four and two thirds minutos for maltais ice 1ne. ironiltnesiir it .i has.

of evaporator units. When a cycle as n frozen-.by @che .thamregfsews illustrated b'y the diagram in time for the ice blocks` tofree 4thenlselves from the surfaces upon which they have been frozen.

lThis assumes that the chart in Fig. be taken inview of Fig. 23 to represent thebjcycle of three evaporator sections, or in other words,` inserting the idle period rafter each freezing period of the chart in Fig; 26. `It also` assumes that `motor 210 is connected in parallel with motor 81 `(Klyig. 3 or 23) to re-'start thermostatically after it has stopped itself at the end of .the /freezingfperiod of one of the evaporatorsections, and' that the switch is kicked off by the 'snap action of part 243 (Fig. 15). b

In further explanationof Figs. -17 `and n 18 it should benoted that the-'shaft 21| maypeextended above the motor (in the case cfa condenslng Aunil'. and control drive in a compartment below the refrigerated space) intofthe refrigerated space to drive the fan280`, which may be provided to circulate the air inthe cabinet for the purpose of keeping a more uniform air temperature and to assist in defrosting or freeing ice as disclosed in myY copending applications above identified. 'I'he shaft 2,80 may belocated invertical position as shown or otherwise as required to actuate valves. shuttersfor control of air flow, etc. It is actuated by the means shown in Fig. 18 from the slow moving shaft 282 by means of the arm 203 and the vspring 284. 'I'he arm 281 on one end (shown as the lower) of shaft 288 is connected with thearm`283 by meansof the spring 2011 with a ball 285 attached to one end of the spring and seated between two prongs of a fork 203 on the outer end of arm 283. This end of spring 233 travels in the circle described by the outer end of the slowly revolving arm 283, causing the arm 201, to which the other end of the spring is attached, to move alternately to positions 281 and 281. At the position shown in Fig. 18the springv 234 would have moveiithearm 281 to the position 281' and sometime before the shaft 282 lhas turned another 180 the spring 280 will cause the arm 201 to move back to the position shown by solid lines. y

It should be noted that the angular movement of the shaft 23B is stopped by the .valve or shutter mechanism to which it is attached and vwhich it operates. In various designs the shaft 288 may be made to actuate the pawl 121 of Figs. 4, 5, or 6; it may be fitted with a crank and pin such as B33 in Fig. 7 and made to operate the connecting rod |80; the shaft 205 of Fig-11 or 250 of Fig. 15 may be an extension of the shaft 282 in Fig. 18, etc. Only a few of the mechanical connections possible between ythe elements of this invention are shown because `these possibilities are too numerous to coverl in' detail, lbut it should be understood that all such combinations are within the scope of my invention. 4

It will be understood that the 'motor 210 of Fig. 17 may be of a horizontal instead of the vertical type shown and that ysuitable. gears would allow the driven shaft282 or the rocker shaft 288 to extend in any direction. The motor rand gear mechanism may be located within the refriger` im space offs magenta-,cabinet if seared.

.. c since theheatoutput of the smallfmotor required isnegligiblor'almostso.` The motor and scar mechanism may be located above or below or at one side of the. refrigerated space, according to the details of design. It is permissible to allow the motor 21,0 to'operate continuously, or it may be wired in 'varend with themotor as er the refrigerating system so that the gear driveis idle whenever the compressor is idle. a *,While the evaporators and ice water tank.

cabinet,y etc., `employed with the present invention may be thesame as disclosed in any of my copending applications mentioned at the beginning of this ,specicatioxn in Figs. 19, 20, and 2l is shown an improved form of ice lwater tank and evaporator particularly suited for use in this connection.

Referring to Fig. l`9the` cabinet 5| will be recognized as a type covered by my previously identined applications. particularly by Serial Number The clearance pocket ||3 in the door for'the water faucet II8'` allows the tank to belocated nearer to the door.` The drain pan and trap construction for disposing of waterassumes use of *the disclosure in my copending application, Serial No. 8,879, medvnebmary 21, 1935.

The tank is here shown equipped with a.

'removablelid 302 which is fitted with a molded rubber gasket 303 embracingits margins to insure a substantially Aair-tight joint with the tank so that breathing of air into and outl of the tank .'may be minimized, protecting thev ice and water within the tank from contamination with food odors and tastes. In order that the cover 302 maybe yheld securely and tightly in place at all times. except when it is lifted for the purposes of adding water to or removing ice from the tank, I have provided the toggle-clamping .means `which Y is described below.

The cover '302 is provided on its upper surface with two ears 304 (304"in'open position) which provide bearings for a shaft which is rigidly connected with two links 301,one on either side of the tank. Each of the two links 301 is hinged to a shorter link 308 by means of a pin which is integral with a knob 300 and the short links 308 are pivotally attached by pin 3 0 to an upright leg of the forward hanger strap 306.

To lift the cover 302 and slide it rearward to the dotted position indicated at 302' one grasps the two knobs 309 and pulls them forward and upward till the shorter links 308 assume the position 308 shown in dotted lines. This causes the .longer links 301 to assume the position 301' which is also shown by dotted lines, moving the ears 304 to the position 304' and the lid 302 to the position 302. In this position the cover is well out of the way, allowing easy access to the tank for removal l of ice, which is accomplished by `means of a percauses the cover to tilt to the position shown by dotted lines when the cover is moved to the 'rear in opening it. The gasket 303 or other suitable soft material is arranged to stop the rearward movement of the cover by striking the closing movement. i cover down on the tank also serves to aid in the rear lining of the cabinet when the cover moves tov the open position, thus protectingthe liningoi the cabinet from damage in the event that the cover is opened quickly.

To close the tank it is only necessary to grasp one or both of the knobs S09 and swing them down to theclcsed position, where the toggle v'locking action of the links S01 and SIS `hold the cover tightly'down on the tank SOI. An

extension of the hinge pin, of which knob S09 is the head, strikes thehanger S96, preventing the toggle levers from goingtoo far over center in This clamping of the holding the tank itself down against the evaporator surfaces SIS (seevFlg. 21) in good thermal contact therewith, since the hinge pins Slt are attached to the hanger S66 and not to the tank.

' previously identified herein. For shipment and handling of the cabinet assembly the tank and cover are securely clamped in position by mere- -ly closing the cover and clamping it with the toggle mechanismshown.

'I'he weight of the tank and its contents and the force exerted downwardly on the tank by the cover clamping means cause the angular surfaces 59 of tank SIII to bear heavily against the evaporator surfaces SI9 on the two sides of the tank. These surfaces SIS are preferably flat and are formed upon the several evaporator units 3I5, .which are individually supported pivotally uon one of the two supporting rods SI2, of w ich there is one on each side of the tank. The rods 3| 2 are rigidly clamped in holes in the hangers 906 by means of set screws SI I, seen in Figs. 20 and 21. The rods SI2 pass through the fins SI1 of the several evaporator units SIS on their respective sides of the tank, but the holes inl ilns 3I1 provide a considerable clearance for the rods SI2, so that each individual evaporator unit is not only free to rock upon its rod 3I2, but may move toward and away e from the tank. A spring SIS, located between each evaporator unit and its rod SI2, urges the surface SI9 against the tank surface 59. 4 In order to provide a more definite thermal break between the evaporator units SI5, fin units 296 are mounted upon the rods SI2 alternately with the evaporator units SII, with springs SIS arranged to urge the fln umts against the wall 59 of tank SIlI in the same manner that the evaporator units are held against the tank.

Whil fins SI1 of the evaporator units are small and are perforated to reduce their area of contact with air, the fins 299 of the fin units 296r are large and are not perforated except by the hole for the lrod SI2. `The iln units SI1 have about the same or even more area of contact with the tank than have evaporator units 3l6,but they have less vertical height adjacent to the tank than have the evaporator units in order that they may be free to rock upon the rod SI2 without contacting either of the manifold tubes 6I or'IS.

A spring seat 299 (Fig. 20) is located on each of the fin units 296 and an embossed spot of part SI! on each 'ofthe evaporator `units SII to receive and retain the corresponding ends of corresponding springs SIS. Figure 19 shows ilve evaporator units SIB and flve flns units 29S on the near (right hand) side of the tank, and there areequal numbers of each on the other side of the tank. `The rear-mostfln unit 29S might be omitted, but it serves to assist in freeing ice frozen by the rear evaporator unit SII. No 11n unit is required or shown in front of the front evaporator unit SI5 because its location is exposed to warmer air than is the rear unit. The main refrigerating effect of evaporator units SI5 is to cool the tank wall and the water within the tank. The fins 296 and theouter surfaces of the tank SIII do most of the cooling of air within the cabinet and the heat pick'd up by flns 296 prevents ice blocks II1 from freezing together and aids in freeing them from the tank wall. l

Althoughthe various evaporator units are connected by means of manifold tubes 6I and SS, these tubes have a certain degree of flexibility so that the springs SIS and the freedom of the evaporator units SI6 to rock upon the rods SI2 insure that each surface SIS makes a good thermal contact with the surface 69 of the tank. This is further aided by lthe fact vthat the tank is made of sheet metal having a certain degree of flexibility and by the water pressure within the tank resulting from the static head 'of water above these surfaces. The fiat surfaces, unlike the conical and spherical surfaces shown in some of my previous applications, allow for a small degree of flexibility which has been found in actual use to be ample for the purpose.

Attention is directed to the form of tank SSI by means of which the top forward lip of the tank allows easy pouring of water into the tank and ready access of floating ice without placing the entire front wall of the tank in such close proximity to the door that an excessive heat transmission from the door to the tank ls allowed. Also the inclination of the rear wall of the tank allows the cover to be short enough to slide out of the way without sacrificing space at the rear of the tank. What little space is left at the rear of the tank and below the path of the cover is utilized for location of control devices such as IIII.

Moisture condensed upon .the tank, tubing and evaporator units drips into the pan 14 at each cycle, since any frost formed is melted during the defrosting period of each cycle. Water is drained from the pan 19 through the trap shown and out of the cabinet through the tube 12, after which it is preferably disposed of by the means disclosed in my copending application Serial Number 8,879, filed February 21, 1935.

Figure 21 shows a baille S I4, which may be empuloyed to direct air currents more definitely over the fins SI1 and to shield the fins from dishes placed in the cabinet. Such bames are shown Supported from the hangers S66 in any suitable manner, allowing a small clearance between the bailles and the ns.

It will be noted that the upper longitudinal corners of the sharp freezer 5l are rounded as indicated in Figs. 19 and^21. This facilitates air flow downward from the ilus and aids in cooling the interior of the cabinet and freeing the ice irozen in the tank from the walls thereof as.'

above described.

Figure 22 illustrates the progressive freezing, rst of several small blocks ||1 of ice on the inner surfaces of the tank Il, and then the larire ice block H1' which is formed by growth and merging of the smaller ice blocks in the event that the freezing cycle is considerably prolonged. When such a large ice block is formed it is found that the ice breaks apart very easily upon lines H5, where the smaller separate blocks join during the latter part of the freezing process to form the larger block. This is the result of a modified crystalline structure of the arate crystalline structures meeting and in freez- A ing together forcing a modified arrangement of crystals at the junction.

Fig, 23 is a. diagrammatic representation of a system employing a triple valve of a type represented by Figs. 11 to 16 inclusive, with three evaporator sections instead of two. The evaporator units 3|5 are in this figure represented by the passages 3|8, which can also be seen in Figs. 2o and 2l, where these evaporating passages or ss are enclosed between the walls 3|! (formed integrally with the fins 3H) and the sheet metal parts 3|9, which are soldered or otherwise attached in a gas-tight manner to the iins or the walls 3N. The tubes Si and @l are soldered to botlgparts and provided with openings for the passage of refrigerant into and out of the evaporating spaces 3N.

In Fig. 23 I have employed the mnnerals 5l to indicate the inlet manifold to one set of evaporating spaces 3|S, with numerals 6|' to indicate the inlet manifold to another set, and bi" indicating the inlet manifolds to the third set of evaporating umts which are arranged in two groups, one on veither side of the tank for convenient utilization of the tank areas Il. The refrigerant circuit is described as follows:

Starting with the compressor 33 the high pressure refrigerant vapor passes through the tube 3l to the condenser 89, where it is condensed to a liquid and flows into the receiver 30. The liquid passes through the tube 9| to the tube 83 and then to therestrictlng device or expansion valve 94 at which point it is reduced in pressure and delivered through the tube to the sharp freezer 5l, where part of -the liquid is evaporated. From the sharp freezer the refrigerant, now partiallyvaporized, goes through the tube 96 to the tubes 326 and 321 since the outlet through the tubes 328 and 329 is blocked at the moment by valves 235 and 236, which are closed. The refrigerant no'w enters the several evaporator units fed by manifolds 6|" and is further vaporized before it flows out through manifolds 63" to the tube 23|. It now enters the valve assembly 230, which is seen in greater detail in Figs. 14, 15, and 16, through the valve port opened by the lifting of the valve 234 from its seat. The heat exchanger between liquid and vapor tubes is omitted in this diagrammatic view as being a detail which is only required under certain conditions and with certain refrigerants,l and being a more or less conventional item.

From the housing of valve assembly 23| the vapor lexits through tube 1| and returns to the suction'side of compressor 33, which is driven bymotor 81. The wiring diagram includes the line conductors |||r and H2 as shown before and the circuit is controlled by the thermostatic control Ill which is seen in detail in Figs. 14 and 15.l This control actuates both the switch and the valve mechanism as before described The mechanical connection between the ratchet wheel or disc 252 (Fig. 23) and the valve as sembly 233 (Fig. 23) maybe'traced in Fig. 15.

One difference between the constructions showninFig.15andFig.23isnotedintheuse of one bulb 26|! in Fig. 15, whereas three-bulbs 32|, 323, and 325 are employed in Fig. 23. As previously explained, the action of control 2li is the same for either of these two arrangef ments, so long as the volatile charge of the control is such that all of the liquid may be contained in one of the bulbs of Fig. 23. There is a slight advantage in the use of three bulbs located remotely from each other in the4 fact that this obviates a certain amount of the overlapping of temperature drops and rises of the three suction tubes in their effects upon the single bulb 23|, but either construction is practicable and can be arranged to produce the desired results.

After the switch of 255 opened and the valves have been'actuated to close the valve 234 and open the valve 23E, and the switch has reclosed, starting the motor 81,. the flow of refrigerant from the tube $8 to the valve assembly 23| is diverted to pass through the tube 323, manifold bl, the evaporating spaces 3|B associated therewith, the manifold 63 and through the port of the valve 235, 'During the next running period of the motor and compressor, this ow will be again diverted to tube 329, mani'- iold 3|". the associated spaces 3|6, manifold and through the port opened by the valve,

The number of evaporatorunits served during each of these three running periods is preferably constant, though not so shown in Fig. 23. It is obvious that the evaporator units might be operated in four groups instead of three. with two groups on each side of the tank and a quadruple valve designed for opening only one of the four valves at a time. Such a quadruple system is considered to be within the scope of this application and so obvious therefrom that no additional drawingls needed to disclose it.

Figs. 24, 25, and 26 are shown for the purpose of explaining in -graphic form the operating cycles of `the various constructions disclosed in the preceding views. Someof these cycles of operation are possible with apparatus which has been disclosed in the copending applications mentioned at the beginning of this specication and there are cycles not illustrated by graphs which are possible with the apparatus herein disclosed, but these graphs should serve to clarify any faults of description or inadvertent omissions of details from my descriptions of the foregoing ilgures.

In Fig. 24 temperatures in degrees Fahrenheit are marked off by horizontal lines in accordance with the scale of figures at the left side of the graph, while time in minutes is indicated by the gures appearing at the top of thegur'e. The broken line A plots variations in temperature of air within the refrigerator employing a control similar to that shown in Fig. ,6 wherein the icemaking cycles and the condensing unit cycles are separately controlled.

The broken line 4B indicates typical temperature variations ofone of the two evaporator sec-v tions or of one of the two suction passages, for instance, the tube 1l of Fig. 6. The solid curve C marks the temperature changes of the other suction passage. for instance, the tube 69 of Fig. 6. The dot and dash line D indicates typical resultant temperature changes of the bulb |40 in Fig. 6.

Starting at the left of Fig. 24 with the downward curve of B resulting from refrigeration in the evaporator section served by the suction tube 10, leading to the open valve in the assembly 15, it will be noted that the temperature drops to about ve degrees, pulling the temperature of the bulb |40 down to slightly below 10 degrees while the temperature of the tube 69, as indicated by the curve C rises to 32 degrees or higher. The drop of bulb temperature causes the valve mechanism (shown in Fig. 6 with reference to Fig. 4) to operate, opening the valve 83 controlling the tube 69 and closing the valve 82 controlling the tube l0. This immediately stops refrigeration of one evaporator section and of the tube 'I0 and starts refrigeration of the other evaporator section and to a lesser degree of the tube 68. This allows the bulb (curve D) to warm up, since it will take several minutes for the frost-back" of the tube 8S to produce much effect upon the temperature of the bulb |60.

The bulb |46 being exposed to air temperature, warms up more rapidly than the tube l@ for eight minutes as shown on the chart, but then the frost-back begins to produce its eifect and the temperature of bulb Mil drops quite rapidly for a few minutes and the curve then ilattens out, falling gradually to the kick-over" temperature of about 9 degrees at the end of the second 20 minute period, which again starts refrigeration in the original evaporator section and the curve B begins to drop.

Without some control of air` temperature within the cabinet, this cycling would go on until the air within the cabinet had been pulled down to so low a temperature that the ice would not be melted free from the surface upon which it is frozen in time to allow for the next freezing cycle on that side of the tank. The result would be that ice would continue to build up on each side of the tank in large blocks which would eventually join in the middle of the tank and make one large piece of ice, which would not be conveniently useable. 'I'his result-is avoided by the use of a. thermostatic control similar to those in common use for controlling refrigerating systems, but in this case operating on cabinet air temperature for the purpose of stopping the condensing unit before the air in the cabinet has dropped to so low a temperature that the ice blocks are in danger of failing to release at each non-freezingl period, while ice is being frozen on the opposite side of the tank.

n the vertical line marked by 90 minutes in Fig. 24 we see that the cabinet air temperature has fallen to about 42 degrees and that at this point the switch was opened by the temperature drop of the bulb |52, causing all of the curves of the graph to assume upward trends. This will continue until the air temperature rises to some predetermined limit, preferably below 50 degrees, at which temperature limit the switch of control |54 re-closes and cycling of the ice-maker will resume at the point it left olf, pulling the curve B downward again on a freezing period which was interrupted by the cutting out of the thermostatic switch and pulling the other curves down more gradually.`

Fig. 23 represents the cyclic operation of a system using a control similar to that illustrated ln Fig. 4, where an idle period of the condensing unit occurs at the end oi' each freezing period on one side of the tank. 'I'his provides a greater period of time for melting the ice free after .each freezing period by utilizing the idle time of the condensing unit between freezing periods instead of having long idle periods of the condensing unit at less frequent intervals.

The coordinates of this graph are similar to those of Fig. 24` except that the time scale is more condensed to show- 240 minutes of operation instead of minutes. The broken line E indicates cabinet air temperature, which is held within closer limits than in Fig. 24. Solid line Fis a curve representing the temperature of one evaporator section; broken line G is the curve of temperature of the other evaporator section: and curve H represents the temperature of control bulb. |03 in Fig; 4.4

Starting with the four curves at the left of Fig. 25 it will be noted that all are rising, indicating that the motor is idle. AtA the end of the first 40 minutes the bulb temperature, as indicated by the curve H, has risen to about 42 degrees, approaching the 44 degree temperature of the air in the cabinet. This isl the cut-ln point of the control and refrigeration starts with the control in the position.r shown in Fig. 4, refrigerating the evaporator section served by the suction tube lll and the open port of the valve 82. Thus, the curve F may be taken as representing the temperature of this evaporator section. This temperature drops rapidly, but ilattens out toward the end of the twenty minute running period, at which time the temperature of tlie bulb |03 has fallen to about nine degrees and the switch |09 opens, stopping the motor and compressor. During this running period the cabinet air temperature has dropped from about 44 degrees to about 42 degrees, but this drop has no appreciable eiect upon the control, which operates upon the temperature of the bulb |03. This bulb temperature approaches, but does not fall so low as the temperature oi' the active evaporator section represented by the curve F.

Now that the refrigerating system has been stopped the temperatures all rise and the bulb (curve H) approaches the temperature of the air in the cabinet, which has in about forty-live minutes of idle time reached approximately 44 degrees again. The bulb, having risen to about 42 degrees causes the bellows |04 to expand, actuating the valve mechanism to open the valve 83 and re-closing the switch |09 to re-start the motor and compressor.

Since the valve has switched to the other side the other evaporator section served by tube 69 will now be refrigerated and curve G will now be caused to drop. At about minutes from the start of the chart we note that curve H has again dropped to the cut-out point and another idle period is initiated.

Ice frozen during the first drop of curve F (a 20 minute period) has 130 minutes in which to free itself from the wall of the tank, since refrigeration is not again started on this side of the tank until the minute line is reached. 'I'he time allowed for melting ice free is the idle time following the freezing plus the freezing time on the other side plus the idle time following the freezing on the other side of the tank. The time will vary according to the rapidity with which the cabinet warms up, cutting down the idle time and the total time for melting the ice free when the weather is warm or considerable warm i'ood 

